TW200403728A - Method to perform deep implants without scattering to adjacent areas - Google Patents
Method to perform deep implants without scattering to adjacent areas Download PDFInfo
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- TW200403728A TW200403728A TW092115308A TW92115308A TW200403728A TW 200403728 A TW200403728 A TW 200403728A TW 092115308 A TW092115308 A TW 092115308A TW 92115308 A TW92115308 A TW 92115308A TW 200403728 A TW200403728 A TW 200403728A
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/04—Manufacture or treatment of semiconductor devices or of parts thereof the devices having at least one potential-jump barrier or surface barrier, e.g. PN junction, depletion layer or carrier concentration layer
- H01L21/18—Manufacture or treatment of semiconductor devices or of parts thereof the devices having at least one potential-jump barrier or surface barrier, e.g. PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic System or AIIIBV compounds with or without impurities, e.g. doping materials
- H01L21/26—Bombardment with radiation
- H01L21/263—Bombardment with radiation with high-energy radiation
- H01L21/265—Bombardment with radiation with high-energy radiation producing ion implantation
- H01L21/26506—Bombardment with radiation with high-energy radiation producing ion implantation in group IV semiconductors
- H01L21/26513—Bombardment with radiation with high-energy radiation producing ion implantation in group IV semiconductors of electrically active species
- H01L21/2652—Through-implantation
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/04—Manufacture or treatment of semiconductor devices or of parts thereof the devices having at least one potential-jump barrier or surface barrier, e.g. PN junction, depletion layer or carrier concentration layer
- H01L21/18—Manufacture or treatment of semiconductor devices or of parts thereof the devices having at least one potential-jump barrier or surface barrier, e.g. PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic System or AIIIBV compounds with or without impurities, e.g. doping materials
- H01L21/26—Bombardment with radiation
- H01L21/263—Bombardment with radiation with high-energy radiation
- H01L21/265—Bombardment with radiation with high-energy radiation producing ion implantation
- H01L21/2658—Bombardment with radiation with high-energy radiation producing ion implantation of a molecular ion, e.g. decaborane
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01L—SEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
- H01L21/00—Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
- H01L21/02—Manufacture or treatment of semiconductor devices or of parts thereof
- H01L21/04—Manufacture or treatment of semiconductor devices or of parts thereof the devices having at least one potential-jump barrier or surface barrier, e.g. PN junction, depletion layer or carrier concentration layer
- H01L21/18—Manufacture or treatment of semiconductor devices or of parts thereof the devices having at least one potential-jump barrier or surface barrier, e.g. PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic System or AIIIBV compounds with or without impurities, e.g. doping materials
- H01L21/26—Bombardment with radiation
- H01L21/263—Bombardment with radiation with high-energy radiation
- H01L21/265—Bombardment with radiation with high-energy radiation producing ion implantation
- H01L21/266—Bombardment with radiation with high-energy radiation producing ion implantation using masks
Abstract
Description
200403728 五、發明說明(1) 發明範疇 本發明關於半導體積體電路,更特定言之係關於要求 雜質深植入之積體電路的製造。 發明背景200403728 V. Description of the invention (1) Scope of the invention The present invention relates to semiconductor integrated circuits, and more specifically to the manufacture of integrated circuits that require deep implantation of impurities. Background of the invention
隨著半導體晶片或一晶圓(例如一矽基板)内之晶粒 的集積度水準提高,對於半導體晶片之製造方法的要求也 越高,例如在半導體基板内製作雜質深植入。今要求較高 劑量的深植入以止住漏洩效應並求取更高的性能和密度。 然而,隨著積體電路之布局將電晶體、電晶體之零件以及 電路之其他組件定位得越來越靠近,要在製造方法中於電 路布局之一區域内進行一深植入變得越來越困難,很容易 侵犯到一鄰近區域且影響該區域的必要參數。由於積體電 路之布局會持續縮小,此問題在未來積體電路的世代中會 變得越來越具關鍵性。As the level of accumulation of crystal grains in a semiconductor wafer or a wafer (for example, a silicon substrate) increases, the requirements for the manufacturing method of the semiconductor wafer also increase, such as making deep implantation of impurities in the semiconductor substrate. Today, higher doses of deep implants are required to stop leakage effects and to achieve higher performance and density. However, as the layout of integrated circuits locates transistors, transistor parts, and other components of the circuit closer and closer, it becomes increasingly necessary to perform a deep implantation in one area of the circuit layout in the manufacturing method. The more difficult it is, it is easy to invade a neighboring area and affect the necessary parameters of the area. As the layout of integrated circuits will continue to shrink, this issue will become increasingly critical in future generations of integrated circuits.
在深植入過程中,欲植入之雜質(在繪出習知技藝之 第2圖和第3圖中以箭頭表示)在植入遮罩(例如光阻劑) 内散射。此遮罩係用來保護吾人不希望在此植入步驟中受 雜質植入之積體電路其他區域。然而,如第3圖所示,在 植入遮罩邊緣會有一些植入雜質散射離開此植入遮罩而進 入晶圓之無遮蔽區域内。此等不想要的雜質散射至鄰近無 遮蔽晶圓區域内會影響製成的積體電路性能且降低一晶圓 内之積體電路晶片的生產良率。 因此,隨著積體電路(特別是需要雜質深植入之積體During the deep implantation process, the impurities to be implanted (indicated by arrows in Figures 2 and 3 where the conventional techniques are drawn) are scattered within the implantation mask (such as a photoresist). This mask is used to protect other areas of the integrated circuit that we do not want to be implanted with impurities during this implantation step. However, as shown in Fig. 3, some implant impurities will scatter away from the implant mask at the edge of the implant mask and enter the unshielded area of the wafer. The scattering of these unwanted impurities into the adjacent unshielded wafer area will affect the performance of the integrated circuit and reduce the production yield of the integrated circuit wafer in a wafer. Therefore, with integrated circuits (especially integrated products that require deep implantation of impurities)
第5頁 200403728 五、發明說明(2) 電路)的密度提高,如何有一克服此等雜質散射至有遮蔽 植入區附近之基板區域内之問題的製程事關重大。因此, 本發明之一目的為設計一種製造需要雜質深植入之積體電 路晶片的製程,其防止雜質散射至有遮蔽植入區附近的基 板區域内。此外,本發明之一目的為對習知深植入方法提 出一簡單改良,此改良不會影響習知深植入方法的生產力 且不會使積體電路晶片之整體製程複雜化。再者,本發明 之一目的為提出一簡單改良使得在深植入步驟之後進行之 習知處理步驟不會因此改良而受到實質影響。 發明 概迷 為達成 間防止 内的製 薄而可 止此等 (ARC : 為人所 反射。 功能為 他材料 點在於 去除光 收集散 業期 區域 在一 且防 塗層 藝中 往回 且其 用其 的優 擇性 成其 以上及其他目的,在依據本發明於一深植入作 雜質從有遮蔽層散射至該有遮蔽區附近之基板 k方法中’在鄰近於有遮蔽植入區之區域内存 輕易去除的散射雜質捕捉層以捕捉散射的雜質 雜質到達晶圓基板。較佳來說該層為一抗反射 ’其一般是定位在一光阻劑的底下且在此技 知是用來防止使光阻劑曝光之訂光從晶圓表面 然而在本發明中,抗反射塗層並非為此而使用 捕捉散射的雜質而非防止反射uv光。儘管可使 (例如一矽酸鹽玻璃的硬遮罩),抗反射塗層 其可在光阻劑接受曝光期間存在,且其能在選 阻劑之後留存且用於本發明的新功能。其在完 射的植入雜質之功能時也相當容易去除。Page 5 200403728 V. Description of the Invention (2) The density of the circuit is increased. How to have a process to overcome the problem of scattering these impurities into the substrate area near the masked implantation area is of great importance. Therefore, an object of the present invention is to design a process for manufacturing an integrated circuit wafer that requires deep implantation of impurities, which prevents the impurities from being scattered into the area of the substrate near the shielding implanted area. In addition, an object of the present invention is to provide a simple improvement to the conventional deep implantation method, which does not affect the productivity of the conventional deep implantation method and does not complicate the overall process of the integrated circuit chip. Furthermore, an object of the present invention is to propose a simple improvement so that the conventional processing steps performed after the deep implantation step are not substantially affected by the improvement. The invention fans can stop this in order to achieve internal prevention of thinning (ARC: reflected by people. The function is to remove other materials. The point is to remove the light collection period and back in the anti-coating technology and use it. Its preference is for its above and other purposes. In the method for scattering impurities from a masked layer to a substrate near the masked area in a deep implant in accordance with the present invention, in the region adjacent to the masked implanted area The scattered impurity capture layer easily removed by the memory to capture the scattered impurity impurities to reach the wafer substrate. Preferably, this layer is an anti-reflection ', which is generally positioned under a photoresist and is used in this technique to prevent The order of light that exposes the photoresist is from the wafer surface. However, in the present invention, the anti-reflection coating is not used for this purpose to capture scattered impurities instead of preventing reflection of UV light. Although it can make (for example, the hardness of a silicate glass Mask), an anti-reflective coating that can exist during the exposure of the photoresist, and it can be retained after the selection of the resist and used for the new function of the present invention. It is also quite equivalent in the function of implanted impurities Easy to go .
第6頁 200403728 五、發明說明(3) 由於散射的植入雜質含有 (1/3)至百分之一(1/100) 角度散射’該捕捉層之厚度得 分之 雖 明非常 於任何 部植入 與基板 起的植 從 解。在 比例綠 清楚顯 (1/3 , 然在深 適於形 深植入 ’雙極 隔開的 入° 以下詳 此要強製。相 示0 )至五十分之一 植入期間利用一 成一 CMOS電晶體 作業,例如高摻 裝置之集極、基 障壁植入,閘摻 細說明參照所附 調的是依慣例該 對地,各特徵的 原始雜質之能量的三分之一 且是以一並非正交於晶圓之 為在深植入雜質之深度之三 (1/50)的範圍内的厚度。 散射雜質離子收集層的本發 之N型井和p型井,其亦能用 雜度源極/汲極和口袋/延伸 極和射極植入,用以將一井 雜之植入以及將井連接在一 圖式能對本發明得到最佳理 等圖式中的各個特徵並非依 尺寸任意地放大或縮小以求 發明詳細說明 以下參照所附圖式詳細說明本發明。第丨圖為一半導 體晶圓10 (在此為矽)的局部剖面圖,該 =渠溝Ua,llb和llc以隔絕欲在製程中形成於晶圓内, 2區。淺渠溝隔絕物(STI)係由反應離子在晶圓内勒 刻出開口且用一絕緣材料12 (例如氧化矽)填充此蝕刻1 ^ (圖中未繪出無填充狀態)的方式形成。為製造一 p s sa體,必須藉由植入適當雜質的方式於晶圓1 〇内形成 P型井和一N型井,例如用硼形成p型井且用磷形成N型井Page 6 200303728 V. Description of the invention (3) Because the scattered implanted impurities contain (1/3) to one hundredth (1/100) of angular scattering, the thickness score of the capture layer is clearly more than that of any part. Removal from implantation with the substrate. It is clearly displayed in the ratio green (1/3, but below the depth suitable for deep implantation of 'bipolar separation'. Details are mandatory below. Phase 0) to one-fifth of the implantation using CMOS Transistor operation, such as the implantation of the collector and base barrier of the high-doping device, the detailed description of the gate doping is based on the conventional adjustment of the ground. One-third of the energy of the original impurity of each feature is Orthogonal to the wafer is a thickness in the range of three (1/50) of the depth of the deep implanted impurities. N-type wells and p-type wells that scatter impurity ion collection layers can also be implanted with heterogeneous source / drain and pocket / extended and emitter electrodes to implant one well and The wells connected in one diagram can obtain the best structure of the present invention. Each feature in the diagram is not arbitrarily enlarged or reduced according to the size for detailed description of the invention. The invention is described in detail below with reference to the drawings. Figure 丨 is a partial cross-sectional view of a half-conductor wafer 10 (here, silicon), which is a trench Ua, llb, and llc to isolate regions 2 to be formed in the wafer during the process. Shallow trench isolation (STI) is formed by etching openings in the wafer with reactive ions and filling the etch 1 ^ with an insulating material 12 (such as silicon oxide) (the unfilled state is not shown in the figure). In order to manufacture a p s sa body, a P-type well and an N-type well must be formed within the wafer 10 by implanting appropriate impurities, such as a p-type well with boron and an N-type well with phosphorus.
200403728 五、發明說明(4) 如第2圖所示,習知技藝形成一P型井1 3之方法為在晶圓i 〇 上沈積一光阻劑1 4 (例如雙氮基奈醌 (di azonaphthoquinone)類型)且將其曝光顯影使得該光 阻劑遮蔽了欲形成P型井1 3處(在此例中為渠溝丨丨a和丨i b 之間)以外的所有地方。硼離子如第2圖中箭頭丨5所示植 入晶圓1 0未受光阻劑遮蔽的區域内。在光阻劑遮蔽區(涵 蓋渠溝lib與11c間之區域以及渠溝ilallb和llc)内,二 箭頭1 5表示之硼離子受光阻劑1 4阻擋,但有一些如第3圖 箭頭1 5 a表示的散射離子,當中一些偏轉至如第3圖之洞1 6 所示的無遮蔽區内。 今參照第4圖和第5圖及一本發明說明,一具備填充了 一絕緣材料(例如氧化矽22 )之淺渠溝隔絕物(sn )渠 溝21a,21b和21c的矽晶圓20塗佈著一薄而易於去除的散^射 雜夤收集層23。層23最好是一抗反射塗層(ARC ),例如 一旋塗玻璃或聚合物,其為此技藝中為人所熟知。一般而 言,層23的厚度會大於3〇 但小於1〇〇〇 nm。層23的^度 係由該層之材料、欲植入之特定雜質及雜質深度來決定^ 整體而言,層23之厚度大約是期望植入深度的三分之一 (1/3)至約五十分之一(1/5〇)。在層23之厚度約大於 30 nm但小於1〇〇〇 _的條件下,以大於8 keV&通常在μ keV至12⑽keV範圍内之能量用删、ι化石朋、或銦進行深 植入。冰植入之硼的劑量得為在丨e丨3至丨^丨6⑽2的範圍 ^、L右该抗反射塗層是沈積成一小於30 nm的厚度,則進 行冰植入的硼此里知低達5 keV。散射雜質離子之能量在200403728 V. Description of the invention (4) As shown in Fig. 2, the method for forming a P-shaped well 13 by conventional techniques is to deposit a photoresist 14 (such as diazonaphthoquinone (di azonaphthoquinone) type) and exposing and developing it so that the photoresist shields all but 13 places (in this example, between trenches 丨 丨 a and ib) where P-wells are to be formed. The boron ions are implanted into the area of the wafer 10 which is not blocked by the photoresist as indicated by arrow 5 in FIG. 2. In the photoresist shielding area (covering the area between the trenches lib and 11c and the trenches ilallb and llc), the boron ions indicated by the two arrows 15 are blocked by the photoresist 14, but some are as shown by the arrow 1 in Figure 3 Some of the scattered ions indicated by a are deflected into the unshielded area shown by hole 16 in Fig. 3. Referring now to FIGS. 4 and 5 and a description of the present invention, a silicon wafer 20 having a shallow trench isolation (sn) trench 21a, 21b, and 21c filled with an insulating material (such as silicon oxide 22) is coated. A thin and easy-to-remove diffused impurity collection layer 23 is provided. Layer 23 is preferably an anti-reflective coating (ARC), such as a spin-on glass or polymer, which is well known in the art. Generally, the thickness of layer 23 will be greater than 30 but less than 1000 nm. The thickness of the layer 23 is determined by the material of the layer, the specific impurities to be implanted, and the depth of the impurities ^ Overall, the thickness of the layer 23 is about one-third (1/3) to about the desired implant depth One-fifth (1 / 5〇). Under the condition that the thickness of the layer 23 is more than about 30 nm but less than 1,000 mm, deep implantation is performed with Zn, ITO, or indium with an energy in the range of more than 8 keV < The dose of boron for ice implantation is in the range of 丨 e 丨 3 to 丨 ^ 丨 6⑽2 ^, L. The anti-reflection coating is deposited to a thickness of less than 30 nm. Up to 5 keV. The energy of scattering impurity ions is
第8頁 200403728 五、發明說明(5) 植入雜質之原始能量的約三分之一(丨/3)至約百分之— (1/1〇G)的範圍内。雖然第4圖和第5圖繪出-P型井之植 入,本發明得用於使用磷或砷或二者進行一 N型井之深植 入。再次在抗反射塗層之厚度為大於3〇⑽但小於1〇〇〇⑽ 的條件下,以大於12 keV且通常在4〇以¥至12〇〇 keV範圍 内之能量用填進行深植入。深植入之磷的劑量得為在5ei2 至1616⑽2的範圍内。再—次’若該抗反射塗層是沈積成 一小於3 〇、⑽的厚度’則進行深植入的磷能量得低達2 二*雖士然、本發明之詳細說明是集中在形成—CM〇S電晶體 =井’本發明亦能用於輕微摻雜的汲極(LDD)以及重 播雜的沒極(H D D ) 的报a、 1 曰X 」的形成。在此等應用中,硼和磷的劑 夏會大於5el4 cm2。 一光阻劑24 (例如說明第2圖和第3圖之習知技藝深植 中使用的類型)力積在層23之頂上。其再次遮蔽渠 ^ 9 g和_2 1 ^間之區域以及渠溝2 1 a,2 1 b和2 1 c。硼離子如箭 5所示植入晶圓20未受光阻劑遮蔽的區域内而形成一p =井26。在光阻劑遮蔽區内,硼離子受光阻劑24阻檔,但 一些如箭頭2 5a表示的散射離子,當中一些偏至 ?之洞27所示的無遮蔽區μ。但不同於第2圖和第3圖之習 1法’如第5圖之箭頭25a或洞27表示的散射離子被捕 f雷Ϊ2日3 =且阻止其到晶圓基板2G,從而保有在晶圓20積 ^電路曰曰片内之製成CM0S電晶體的性能。在形成p型井之 北ο去除光阻劑24且在欲形成N型井期間再次施加以遮蔽P 6。在完成所有深植入作業之前最好讓層2 3保留在晶Page 8 200403728 V. Description of the invention (5) The original energy of implanted impurities is in the range of about one-third (丨 / 3) to about one-tenth (1 / 1G). Although Figures 4 and 5 depict the implantation of a -P well, the present invention can be used for deep implantation of an N-well using either phosphorus or arsenic or both. Once again, under the condition that the thickness of the anti-reflective coating is greater than 30 ⑽ but less than 10,000 ⑽, deep implantation is performed with filling at an energy of more than 12 keV and usually in the range of ¥ 40 to 12,000 keV. . The dose of deep implanted phosphorus is in the range of 5ei2 to 1616⑽2. Again—'If the anti-reflection coating is deposited to a thickness of less than 30 ⑽, then the phosphorus energy for deep implantation is as low as 2 2 * Although it is true, the detailed description of the present invention is focused on the formation—CM The transistor can be used in the formation of a lightly doped drain (LDD) and a replayed hybrid anode (HDD). In these applications, boron and phosphorus agents are larger than 5el4 cm2. A photoresist 24 (for example, illustrating the type used in the conventional technique of deep planting of Figs. 2 and 3) is forced on top of the layer 23. It again covers the area between the channels ^ 9 g and _2 1 ^ and the channels 2 1 a, 2 1 b and 2 1 c. The boron ions are implanted into the area of the wafer 20 not covered by the photoresist as shown by arrow 5 to form a p = well 26. In the photoresist shielding area, boron ions are blocked by the photoresist 24, but some of the scattered ions shown by the arrow 25a, some of them are biased to the unshielded area μ shown by the hole 27 of?. However, it is different from the method 1 in Figures 2 and 3 'The scattered ions indicated by the arrow 25a or hole 27 in Figure 5 are captured f thunder 2 3 = and prevent it from reaching the wafer substrate 2G, so that it remains in the crystal The performance of the CM0S transistor made of a 20-inch circuit is described in the chip. North of the formation of the p-type well, the photoresist 24 is removed and applied again to mask P 6 during the formation of the N-type well. It is best to leave layers 2 3 in the crystals before completing all deep implant operations
第9頁 200403728 五、發明說明(6) 圓20上。 第4圖和第5圖中已顯示層23是在光阻劑24的下層,但 其並不一定是出現在光阻劑底下。層2 3僅只必須覆蓋渠溝 21a與21b之間的區域。然而,將層23侷限為僅在此區會造 成額外步驟,為求簡化本發明之方法是將層2 3沈積在整個 晶圓上。此外,前文已提及抗反射塗層為層2 3之較佳材 料,得以一包含矽酸鹽玻璃〔例如硼矽酸玻璃/四乙氧基 矽酸鹽(BSG/TE0S )〕之硬遮罩取代抗反射塗層。不同於 抗反射塗層之沈積方法為旋塗法,硼矽酸玻璃/四乙氧基 矽酸鹽是由化學氣相沈積法(CVD )沈積。雖然沒有要土 ίL有:f乳化矽層(圖中未示)#在於雜質離子捕捉 層23 (例如抗反射塗層及硬遮罩層)底下。 第6圖和第7圖顯示在沒有(第6圖)和有(第7圖)本 ”離子捕捉層23 (第4圖—第5圖)的條件下進行 = 植:模為散射離開州 :學匕圖…質且的 此一圖之左手邊上的條棒是 中沒有層23 (第4圖_第5二朋:广辰度的尺標。在第6圖 ^ 0 ^ 5圖)的條件下,圖φ LV告<、n 溝隔絕物(ST I )上方之浐為w Η中以罪近淺渠 提高濃产F岡埒封认 劑邊緣的圓圈標出的硼離子 杈问/辰度&因散射的雜質硼離子 J朋雕卞 此硼離子提高濃度區從抗蝕劑邊緣:見。從圖中可見 一 180 nm之本發明硬遮罩層的 、、· Am,而在有 到此硼離子提高濃度區的存為,石夕晶圓内即看不 200403728 五、發明說明(7) 高的離子濃度的優點在於一窄小的場效電晶體(FET )不 管是否位在抗蝕劑邊緣都會具有幾乎恆定的閾值,此等場 效電晶體是當今及未來用來使積體電路之密度提高的設 計。其好處是使製成的晶圓有提高的積體電路晶片良率。 儘管已就特定實施例說明本發明,熟習此技藝者會瞭 解到可不脫離所附申請專利範圍所定義之本發明精神和範 圍做出許多變化和修改。章節結束Page 9 200403728 V. Description of Invention (6) Circle 20. It has been shown in Figs. 4 and 5 that the layer 23 is under the photoresist 24, but it does not necessarily appear under the photoresist. The layers 2 3 only have to cover the area between the trenches 21a and 21b. However, limiting layer 23 to only this region would result in additional steps. To simplify the invention, the method is to deposit layers 23 on the entire wafer. In addition, the antireflective coating has been mentioned above as the preferred material for layer 23, so that a hard mask containing silicate glass (eg, borosilicate glass / tetraethoxysilicate (BSG / TE0S)) can be used. Replaces anti-reflective coating. Unlike the anti-reflection coating, which is spin-on, borosilicate glass / tetraethoxy silicate is deposited by chemical vapor deposition (CVD). Although not required, there are: an emulsified silicon layer (not shown in the figure) # under the impurity ion trap layer 23 (such as an anti-reflection coating and a hard mask layer). Figures 6 and 7 show the absence (Figure 6) and the presence (Figure 7) of the present "ion trap layer 23 (Figure 4-Figure 5) = planting: mode for scattering away from the state: Learn the dagger picture ... The bar on the left-hand side of this picture is without layer 23 (picture 4_5 second friend: the scale of Guangchen degree. Picture 6 ^ 0 ^ 5) Under the conditions, the figure φ LV tells that the 上方 above the n-ditch barrier (ST I) is w. The boron ion branch marked by the circle near the edge of the sealant to increase the concentration of F. Chen Du & Because of the scattered impurity boron ions, J. This boron ions increase the concentration region from the edge of the resist: see. From the figure, it can be seen that a 180 nm hard mask layer of the present invention, and Am With the existence of the boron ion increasing concentration region, it cannot be seen in the Shi Xi wafer. 200403728 V. Description of the invention (7) The advantage of high ion concentration is that a narrow field-effect transistor (FET) is not located in The resist edges will have almost constant thresholds. These field effect transistors are designs used today and in the future to increase the density of integrated circuits. The benefit is that the fabricated Improved yield of integrated circuit wafers. Although the invention has been described in terms of specific embodiments, those skilled in the art will recognize that many changes and modifications can be made without departing from the spirit and scope of the invention as defined by the scope of the appended patents. End of chapter
第11頁 200403728 圖式簡單說明 第1圖為一含有欲在積體電路製程中活性化之淺渠溝隔絕 物區之習知技藝半導體晶圓的局部剖面圖。 第2圖為第1圖習知技藝半導體晶圓之剖面圖,其中晶圓之 局部於雜質深植入期間受一光阻劑遮蔽而形成一 P型井。 第3圖為第2圖習知技藝半導體晶圓之局部的剖面放大圖, 圖中顯不在晶圓基板内受遮敝晶圓部分附近的散射雜質離 子。Page 11 200403728 Brief Description of Drawings Figure 1 is a partial cross-sectional view of a conventional semiconductor wafer containing a shallow trench isolation area to be activated in the integrated circuit manufacturing process. FIG. 2 is a cross-sectional view of the conventional semiconductor wafer of FIG. 1, in which a part of the wafer is masked by a photoresist during deep implantation of impurities to form a P-well. FIG. 3 is an enlarged cross-sectional view of a part of the conventional semiconductor wafer of FIG. 2. The figure shows scattered impurity ions that are not in the vicinity of the portion of the wafer substrate that is blocked by the wafer.
第4圖為第1圖習知技藝半導體晶圓的剖面圖,其中晶圓整 體有一本發明之薄而易於去除的雜質捕捉層,且其中晶圓 之局部於雜質深植入期間受一光阻劑遮蔽而形成一 P型 井。 第5圖為第4圖半導體晶圓之局部的剖面放大圖,其中顯示 在晶圓受遮蔽部分附近之本發明層内的散射雜質離子。 第6圖為一沒有散射離子捕捉層之散射植入硼離子的蒙特 卡羅模擬(Monte Carlo simulation)結果圖。 第7圖為一有一散射離子捕捉層之散射植入硼離子的蒙特 卡羅模擬結果圖。 元件符號說明:FIG. 4 is a cross-sectional view of the conventional semiconductor wafer of FIG. 1. The wafer as a whole has a thin and easy-to-remove impurity trap layer according to the present invention, and a part of the wafer is subjected to a photoresist during the deep implantation of impurities. The agent was masked to form a P-shaped well. Fig. 5 is an enlarged cross-sectional view of a part of the semiconductor wafer of Fig. 4, which shows scattered impurity ions in the layer of the present invention in the vicinity of the shielded portion of the wafer. Fig. 6 is a Monte Carlo simulation result diagram of a boron ion implanted without a scattering ion trap layer. Figure 7 is a Monte Carlo simulation result of a boron ion implanted with a scattering ion trap layer. Component symbol description:
1 0、2 0 晶圓 1 1 a、1 1 b、11 c、2 1 a、2 1 b、2 1 c 淺隔絕物渠溝 12 絕緣材 料 14 、24 光 阻劑 16 、2Ί 洞 23 層 13、26 P型井 1 5、1 5 a 箭頭 22 氧化矽 2 5、2 5 a 箭頭1 0, 2 0 Wafer 1 1 a, 1 1 b, 11 c, 2 1 a, 2 1 b, 2 1 c Shallow insulation trenches 12 Insulating materials 14, 24 Photoresist 16, 16 Holes 23 Layers 13 , 26 P-type well 1 5, 1 5 a arrow 22 Silicon oxide 2 5, 2 5 a arrow
第12頁Page 12
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DE10138648A1 (en) * | 2001-08-07 | 2003-03-06 | Infineon Technologies Ag | Method for producing a MOS transistor and a bipolar transistor in parallel |
DE10356668B4 (en) * | 2003-12-04 | 2005-11-03 | Infineon Technologies Ag | Manufacturing method for a hard mask on a semiconductor structure |
US7824933B2 (en) * | 2005-03-08 | 2010-11-02 | International Business Machines Corporation | Method of determining n-well scattering effects on FETs |
US7550787B2 (en) | 2005-05-31 | 2009-06-23 | International Business Machines Corporation | Varied impurity profile region formation for varying breakdown voltage of devices |
US7709345B2 (en) * | 2006-03-07 | 2010-05-04 | Micron Technology, Inc. | Trench isolation implantation |
US7598130B2 (en) * | 2006-09-28 | 2009-10-06 | Taiwan Semiconductor Manufacturing Company, Ltd. | Method for reducing layout-dependent variations in semiconductor devices |
US8034699B2 (en) * | 2009-05-12 | 2011-10-11 | International Business Machines Corporation | Isolation with offset deep well implants |
US20100330756A1 (en) * | 2009-06-25 | 2010-12-30 | International Business Machines Corporation | Integrated circuit structure manufacturing methods using hard mask and photoresist combination |
US20110049582A1 (en) * | 2009-09-03 | 2011-03-03 | International Business Machines Corporation | Asymmetric source and drain stressor regions |
US8482076B2 (en) | 2009-09-16 | 2013-07-09 | International Business Machines Corporation | Method and structure for differential silicide and recessed or raised source/drain to improve field effect transistor |
US8106462B2 (en) * | 2010-01-14 | 2012-01-31 | International Business Machines Corporation | Balancing NFET and PFET performance using straining layers |
US8299545B2 (en) * | 2010-01-28 | 2012-10-30 | International Business Machines Corporation | Method and structure to improve body effect and junction capacitance |
US8421181B2 (en) | 2010-07-21 | 2013-04-16 | International Business Machines Corporation | Schottky barrier diode with perimeter capacitance well junction |
US8445969B2 (en) | 2011-04-27 | 2013-05-21 | Freescale Semiconductor, Inc. | High pressure deuterium treatment for semiconductor/high-K insulator interface |
KR102108175B1 (en) * | 2013-12-27 | 2020-05-08 | 삼성전자주식회사 | Methods of manufacturing a semiconductor device |
KR102222818B1 (en) * | 2014-10-06 | 2021-03-04 | 삼성전자주식회사 | Methods of manufacturing a semiconductor device |
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US4089103A (en) * | 1976-06-04 | 1978-05-16 | Honeywell Inc. | Monolithic integrated circuit device construction methods |
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US4224733A (en) * | 1977-10-11 | 1980-09-30 | Fujitsu Limited | Ion implantation method |
JPH0797566B2 (en) * | 1987-03-23 | 1995-10-18 | 日本電気株式会社 | Method for manufacturing semiconductor device |
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US5935867A (en) * | 1995-06-07 | 1999-08-10 | Advanced Micro Devices, Inc. | Shallow drain extension formation by angled implantation |
JP3137077B2 (en) * | 1998-06-16 | 2001-02-19 | 日本電気株式会社 | Semiconductor device and manufacturing method thereof |
WO2002089196A2 (en) * | 2001-04-28 | 2002-11-07 | Koninklijke Philips Electronics N.V. | Trench-gate semiconductor devices and their manufacture |
US6610585B1 (en) * | 2002-02-26 | 2003-08-26 | International Business Machines Corporation | Method for forming a retrograde implant |
US6667205B2 (en) * | 2002-04-19 | 2003-12-23 | International Business Machines Machines Corporation | Method of forming retrograde n-well and p-well |
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